DRIVES WITH PARTIAL CYCLOID TEETH PROFILE
CROSS REFERENCE TO RELATED APPLICATION
[0001] The present application claims priority to U.S. Provisional patent application number 62/152,484, filed on April 24, 2015, and entitled "Drives with Partial Cycloid Teeth Profile," which is herein incorporated by reference as if fully set forth in this description.
BACKGROUND
[0002] A transmission is a machine that converts the speed and torque from power source to a different speed and torque provided to an output, where the product of speed and torque on the input equals the product of the speed and torque on the output, less any power inefficiencies in the transmission. The term "transmission" may refer generally to a gearbox that uses gears and gear trains to provide speed and torque conversions from a rotating power source to another device. Industrial machinery, medical robotics, and domestic electronics may utilize such transmissions. Selecting or designing a transmission involves considering multiple factors. Example factors include load capacity, gear ratio, and cost.
SUMMARY
[0003] The present disclosure describes embodiments that relate to systems and apparatuses associated with drives with partial cycloid teeth profile.
[0004] In one aspect, the present disclosure describes an apparatus. The apparatus includes a ring gear having an open annular space and a plurality of gear teeth disposed on an interior peripheral surface thereof. Each of the plurality of gear teeth of the planet gear has a partial cycloid profile, and the ring gear is fixed. The apparatus also includes a planet gear rotatable within the open annular space of the ring gear. The planet gear has a plurality of gear teeth on an exterior periphery thereof, and each of the plurality of gear teeth of the planet gear has a partial cycloid profile. The planet gear has a total number of gear teeth and the ring gear has a total number of gear teeth, with the total number of gear teeth of the planet gear being smaller than the total number of gear teeth of the ring gear. The gear teeth of the planet gear operatively mesh with corresponding gear teeth of the ring gear. The total number of gear teeth of the planet gear provides each gear tooth of the planet gear with a bending strength and a compressive strength such that the bending strength and the compressive strength differ by less than a predetermined amount.
[0005] In another aspect, the present disclosure describes a cycloid drive. The cycloid drive includes an input shaft and a bearing eccentrically mounted to the input shaft. The cycloid drive also includes a ring gear having an open annular space and a plurality of gear teeth disposed on an interior peripheral surface thereof. Each of the plurality of gear teeth of the planet gear has a partial cycloid profile, and the ring gear is fixed. The cycloid drive also includes a planet gear mounted to the eccentrically mounted bearing and rotatable within the open annular space of the ring gear. The planet gear has a plurality of gear teeth on an exterior periphery thereof, and each of the plurality of gear teeth of the planet gear has a partial cycloid profile. The planet gear rotates eccentrically with respect to rotation of the input shaft. The planet gear has a total number of gear teeth and the ring gear has a total number of gear teeth, with the total number of gear teeth of the planet gear being smaller than the total number of gear teeth of the ring gear. The gear teeth of the planet gear operatively mesh with corresponding gear teeth of the ring gear. The total number of gear teeth of the planet gear provides each gear tooth of the planet gear with a bending strength and a compressive strength such that the bending strength and the compressive strength differ by less than a predetermined amount.
[0006] The foregoing summary is illustrative only and is not intended to be in any way limiting. In addition to the illustrative aspects, embodiments, and features described above, further aspects, embodiments, and features will become apparent by reference to the figures and the following detailed description.
BRIEF DESCRIPTION OF THE FIGURES
[0007] Figure 1 illustrates a cycloid generated by a rolling circle, in accordance with an example implementation.
[0008] Figure 2A illustrates an epicycloid and a hypocycloid obtained by rolling a small circle on a circumference of a bigger circle, in accordance with an example implementation.
[0009] Figure 2B illustrates the epicycloid of Figure 2A separately, in accordance with an example implementation.
[0010] Figure 2C illustrates the hypocycloid of Figure 2A separately, in accordance with an example implementation.
[0011] Figure 2D illustrates a cycloid gear with three teeth having a full cycloid profile, in accordance with an example implementation.
[0012] Figure 2E illustrates a gear tooth with a partial cycloid profile, in accordance with an example implementation.
[0013] Figures 3A, 3B, 3C, 3D, 3E, and 3F illustrate operation of a cycloid drive, in accordance with an example implementation.
[0014] Figures 4A, 4B, 4C, and 4D illustrate a cycloid drive with partial cycloid teeth, in accordance with an example implementation.
[0015] Figure 5 illustrates the effect of using partial cycloid teeth on load capacity, in accordance with an example implementation.
[0016] Figure 6A illustrates rolling contact diameter, in accordance with an example implementation.
[0017] Figure 6B illustrates a cycloid drive with rolling contact diameter passing through a midpoint of cycloid segments of partial cycloid teeth, in accordance with an example implementation.
[0018] Figure 7 illustrates a mechanism that compensates for eccentric motion of an output shaft of a cycloid drive, in accordance with an example implementation.
[0019] Figure 8 illustrates a coupling used to connect two shafts that are not aligned coaxially, in accordance with an example implementation.
[0020] Figures 9A and 9B illustrate a coupling configuration to compensate for eccentricity at an output of a cycloid drive, in accordance with an example implementation.
[0021] Figures 10A and 10B illustrate a configuration to compensate for eccentricity at an output of a cycloid drive, in accordance with an example implementation.
[0022] Figure 11 illustrates another configuration to compensate for eccentricity of a cycloid drive, in accordance with an example implementation.
DETAILED DESCRIPTION
[0023] The following detailed description describes various features and functions of the disclosed systems and methods with reference to the accompanying figures. The illustrative system and method embodiments described herein are not meant to be limiting. It may be readily understood that certain aspects of the disclosed systems and methods can be arranged and combined in a wide variety of different configurations, all of which are contemplated herein.
[0024] Further, unless context suggests otherwise, the features illustrated in each of the figures may be used in combination with one another. Thus, the figures should be generally viewed as component aspects of one or more overall implementations, with the understanding that not all illustrated features are necessary for each implementation.
[0025] Additionally, any enumeration of elements, blocks, or steps in this specification or the claims is for purposes of clarity. Thus, such enumeration should not be interpreted to require or imply that these elements, blocks, or steps adhere to a particular arrangement or are carried out in a particular order.
I. Overview
[0026] Selecting or designing a transmission for a particular application involves considering multiple factors. Example factors include load capacity, gear ratio, and cost Transmission systems could be heavy if a large load capacity is required. On the other hand, small transmission systems tend to have a small load capacity. Further, transmission systems tend to be expensive if high performance, defined by parameters such as efficiency, backlash, etc., is needed. Hence, a transmission system that increase load capacity for a given volume and reduce the cost of manufacturing is desired.
[0027] A cycloid drive or cycloid speed reducer is a mechanism for reducing the speed of an input shaft by a certain ratio. When compared to other similar speed reducers, cycloid drives are capable of relatively high speed reduction ratios in compact sizes, high stiffness and load capacity, low inertia, and little to no backlash. However, load capacity of cycloid drives may be limited by mechanical factors such as wear and tear. Additionally, as described below, cycloid drives involve eccentric gear systems, and compensating for the eccentricity of the gear systems may involve using a large number of parts along with requiring precision manufacturing techniques.
[0028] Disclosed herein are gear systems that improve load capacity of cycloid drives by using gear teeth that have a partial cycloid profile. Further, the disclosed systems utilize configurations having a reduced number of parts to harvest the output of the cycloid and compensate for inherent eccentricity of cycloid drives.
II. Cycloid Gears
[0029] A cycloid is the curve traced by a point on a rim of a circular wheel as the wheel rolls along a straight line without slippage. Figure 1 illustrates a cycloid 100 generated by a rolling circle 102, in accordance with an example implementation. A point 104 on a rim of
the circle 102 traces a curve, the cycloid 100, as the circle 102 moves along a surface 106 in a direction of arrow 108.
[0030] A cycloidal gear has a cycloid profile rather than an involute gear profile used for most other gears. Teeth of cycloid gears have the shape of cycloids obtained by rolling (without sliding) an imaginary small circle on a circumference of a main circle. A curve traced by a virtual point fixed on a small circle forms a cycloid. If the small circle rolls outside of the main circle, its point will trace an epicycloid. If the point rolls inside the main circle, the curve will be a hypocycloid.
[0031] Figure 2A illustrates an epicycloid 200 and a hypocycloid 202 obtained by rolling a small circle on a circumference of a bigger circle, in accordance with an example implementation. The epicycloid 200 is shown as a solid line, whereas the hypocycloid 202 is shown as a dashed line. The epicycloid 200 is traced by a point of a small circle, when it rolls outside the bigger circle, and the hypocycloid 202 is traced by the point when it rolls inside the bigger circle. Figure 2B illustrates the epicycloid 200 separately and Figure 2C illustrates the hypocycloid 202 separately, in accordance with an example implementation.
[0032] A cycloid gear can be constructed by interleaving the epicycloid 200 with the hypocycloid 202 at their intersection points (on the main circle). Figure 2D illustrates a cycloid gear 204 with three teeth 206A, 206B, and 206C having a full cycloid profile, in accordance with an example implementation. Three teeth are shown in Figure 2D as an example for illustration, and a smaller or larger number of teeth could be used.
[0033] The cycloid gear 204 is constructed by interleaving portions of the epicycloid 200, such as portion 208 with portions of the hypocycloid 202 such as portion 210 at their intersection points such as point 212. The resulting teeth 206A, 206B, and 206C are referred to as having a full cycloid profile because the portions taken from the epicycloid 200 and the hypocycloid 202 are full segments between interesting point between the epicycloid 200 and the hypocycloid 202. For instance, the portion 208 is a full segment of the epicycloid 200 between the intersection point 212 and intersection point 214 with the hypocycloid 202.
[0034] As described below, the load capacity of a cycloid drive may be enhanced by using a cycloid gear with teeth having a partial cycloid profile. Figure 2E illustrates a gear tooth 216 with a partial cycloid profile, in accordance with an example implementation. The gear tooth 216 with a partial cycloid profile can be constructed by augmenting segments of the full cycloid profile. For instance, a segment 218 shown in Figure 2D between lines 220 A and
220B could be augmented with a segment 222 between lines 224 A and 224B. Thus, the resulting tooth 216 has a partial cycloid profile instead of the full cycloid profile of the teeth 206A-C.
[0035] Using teeth such as the tooth 216 having a partial cycloid profile facilitates making cycloid gears having more numerous, but thinner gear teeth, as described below with respect to Figures 4A-4D. Advantages of using such gears are described below with respect to Figure 5.
III. Example Cycloid Drive Systems
[0036] Figures 3A-3F illustrate operation of a cycloid drive 300, in accordance with an example implementation. As shown in Figure 3A, the cycloid drive 300 includes (i) a ring gear 302 having an open annular space 303, (ii) a planet gear 304 rotatable within the open annular space 303 of the ring gear 302, (iii) an input shaft 306, which is concentric with the ring gear 302, and (iv) an eccentric drive member 308, which is coupled to the input shaft 306 and the planet gear 304.
[0037] As shown in Figure 3A, and as an example for illustration, the planet gear 304 has five teeth or lobes, such as tooth 310 disposed on an exterior periphery of the planet gear 304, whereas the ring gear 302 has six teeth or lobes disposed on an interior peripheral surface of the ring gear 302. Thus, a number of gear teeth of the planet gear 304 is smaller than a number of gear teeth of the ring gear 302, and the gear teeth of the planet gear 304 operatively mesh with corresponding gear teeth of the ring gear 302. The terms "lobes" and "teeth" are used interchangeably in this disclosure.
[0038] The input shaft 306 is rotated in the direction of a solid arrow shown in Figure 3 A (i.e., clockwise direction). The input shaft 306 is coupled to the eccentric drive member 308, and thus imparts an eccentric motion to the planet gear 304. This is illustrated by a point marker 312 and a dashed arrow 314. As the input shaft 306 is rotated, Figures 3B-3F illustrate how the point marker 312 moves. The locus of the point marker 312 is illustrated by the dashed arrow 314. This eccentric motion is minimized or eliminated by an output mechanism prior to harvesting the output. The output mechanism is not illustrated in Figures 3A-3F, but example output mechanism will be described below.
[0039] Generally, load capacity of the cycloid drive 300 depends on bending strength and the compressive strength of each lobe of the planet gear 304 as it meshes with the lobes of the ring gear 302. In other words, the load capacity of the cycloid drive 300 is limited by the
stresses induced by bending loads acting on the teeth. The load capacity is also limited by the Hertzian contact stresses where the planet lobes contact the ring gear lobes.
[0040] To improve load capacity of a cycloid drive, disclosed herein is a cycloid drive with a larger number of teeth that are smaller in size compared to teeth of the cycloid drive 300, but of the same gear ratio as the cycloid drive 300. As mentioned above with respect to Figure 2E, to increase the number of teeth and make them smaller, segments of the full cycloidal profile could be used to make the teeth. In other words, smaller teeth may be made using segments of the full cycloid profile. A gear tooth that uses a segment of the full cycloid profile may be referred to as a partial cycloid tooth. Height of a partial cycloid tooth may be made as small as desired. This type of tooth profile has the advantage of increasing the contact stress load capacity of the cycloid drive, i.e., by increasing the number of contact points loaded in compression, and thus increasing the compressive strength of cycloid drive.
[0041] Figures 4A-4D illustrate a cycloid drive with partial cycloid teeth, in accordance with an example implementation. Figure 4A shows a planet gear 400 with large lobes or teeth, which is similar to the planet gear 304. One such tooth is tooth 402. Also shown in Figure 4A is another planet gear 404 that has smaller teeth, such as tooth 406. The profile of teeth of the planet gear 404 is a segment of the full cycloidal tooth, i.e., partial cycloid profile, thus enabling the planet gear 404 to have a larger number of teeth.
[0042] As shown in Figure 4A, the shape of the profile of smaller teeth matches the shape of a segment of the larger teeth. For instance, portion labeled 408 is common to the smaller tooth 406 and the larger tooth 402. Thus, while the tooth 402 is a full cycloid tooth, the tooth 406 is a partial cycloid tooth, whose profile is a segment (e.g., similar to the segments 218 and 222) of the profile of the tooth 402.
[0043] The teeth on a ring gear may be adjusted in a similar manner. Figure 4B shows a ring gear 410 that could have full cycloid gear teeth such as gear tooth 412 to match full cycloid gear teeth such as the tooth 402 of the planet gear 400. Alternatively, the ring gear 410 could have partial cycloid gear teeth such as gear tooth 414 to match partial cycloid gear teeth such as the tooth 406 of the planet gear 404.
[0044] Figure 4C illustrates the planet gear 400 and the ring gear 410 where each gear has full cycloid teeth, whereas Figure 4D illustrates the planet gear 404 and the ring gear 410 where each gear has partial cycloid teeth. The teeth may be made as small as desired by using partial cycloid profiles instead of a full cycloid profile. Using partial cycloid teeth
allows for using a larger number of smaller teeth, which improves load capacity of the cycloid drive as described next.
[0045] Load capacity of the cycloid drive may be increased by matching the bending strength with the compressive strength of the gear teeth. To match the bending strength and the compressive strength, thickness of a tooth may be reduced, while increasing the number of teeth. Reducing thickness of the tooth reduces the bending strength load capacity of the drive. On the other hand, increasing the number of teeth increases the compressive strength load capacity of the drive as the load is now distributed over a larger number of teeth. For example, the thickness and the number of teeth may be adjusted such that each tooth has a bending strength and a compressive strength that differ by less than a predetermined amount (e.g., differ by less than by 5%, differ by less than 10%, or differ by less than some other amount). Matching the bending strength and compressive strength of the gear teeth in this way may maximize or increase the load capacity of the cycloid drive.
[0046] Figure 5 illustrates the effect of using partial cycloid teeth on load capacity, in accordance with an example implementation. Solid line 500 depicts relationship between the bending strength and the compressive strength. The relationship is illustrated as linear for illustration only; however, the relationship could take other nonlinear shapes.
[0047] In determining bending stress on a gear tooth, the gear tooth could be modeled as a cantilever beam. The bending stress could thus be determined by the following simplified equation:
FY
(1)
where Wt is a tangential load at a tip of the tooth, Pd is the diametrical pitch, F is the face width of the tooth, and Y is the dimensionless Lewis form factor.
[0048] Thus, as shown by equation (1), the bending stress on a gear tooth is inversely proportional to the Lewis form factor. The Lewis form factor generally takes into account several geometry factors, including stress concentration, and increases as the number of teeth increases. Thus, the thicker and less numerous the teeth are, the lower the Lewis factor, the lower the bending stress, and thus the higher the bending strength of the tooth, and vice versa.
[0049] The compressive stress on a gear tooth is proportional to the Hertzian contact pressure, which could be determined by the following simplified equation:
2 F cos r2
(2)
where p is the Hertzian contact pressure, E* is an effective modulus of elasticity, φ is pressure angle, ri and r2 are the equivalent radii equal to pitch radius of each gear of two meshing gears multiplied by sin (φ). The pressure angle φ is the angle between the tooth face and the gear wheel tangent. In other words, it is the angle at a pitch point between the line of pressure (which is normal to the tooth surface) and the plane tangent to the pitch surface. The pressure angle indicates the direction normal to the tooth profile.
[0050] As indicated by equation (2), the compressive stress on a gear tooth is inversely proportional to cosine of the pressure angle. The pressure angle is larger for bigger and thicker teeth, while smaller teeth are characterized by a reduced pressure angle. Thus, the thicker the tooth, the larger the pressure angle, the higher the compressive stress, and thus the lower the compressive strength of the tooth. Also, thicker less numerous teeth indicate a decreased compressive strength as the load is distributed over a smaller number of teeth.
[0051] Therefore, a thick or full cycloid tooth (e.g., the tooth 402) may be represented by points such as point A on the line 500 of Figure 5. At point A, the compressive strength is low, whereas the bending strength is high. On the other hand, points such as point B represent low bending strength and high compressive strength. Both of these two operating points A and B represent a reduced load capacity. The load capacity of the drive is limited by whichever of the compressive strength and bending strength is lower.
[0052] To improve the load capacity of the cycloid drive, the bending strength and the compressive strength should be more balanced such that they are equal or within a threshold value of each other. This is depicted by point C. Points such as C are achieved by reducing the tooth thickness and increasing the number of teeth as illustrated by the planet gear 404 having the gear tooth 406 and the ring gear 410 having gear teeth such as the tooth 414 (as opposed to the tooth 412). The configuration represented by the planet gear 404 and the ring gear 410 having gear teeth such as tooth 414 aims to achieve operating points such as point C.
[0053] In addition to the improved drive load capacity, another advantage of the partial cycloid teeth is that the effective pressure angle between the planet gear and the ring gear is reduced, as is the sliding distance. Reducing sliding distance and pressure angle may increase the efficiency of the cycloid drive.
[0054] The propensity of the gears to slide may be depicted by an imaginary line called the "rolling contact diameter." Figure 6A illustrates rolling contact diameter, in accordance with an example implementation. The rolling contact diameter for a planet gear 600 is shown by a line 602, and the rolling contact diameter for a ring gear 604 is shown by a line 606. The further away the point of contact between the gears is from the rolling contact diameter, the larger the velocity with which the gears are sliding across one another during meshing. When the teeth contact precisely at the rolling contact diameters, only rolling contact occurs, and the teeth do not slide relative to each other.
[0055] The amount of sliding loss is reduced if the cycloid drive has partial cycloid teeth, and the rolling contact diameter passes through the cycloid segments of the partial cycloid teeth. Particularly, the sliding loss is minimized if the rolling contact diameter is centered in, or passes through a middle point of, the cycloid segments of the partial cycloid teeth. Thus, to reduce sliding loss, the number of gear teeth should be selected such that the rolling contact diameter passes through, or within a threshold distance from, the midpoint of the cycloidal segment. The threshold distance may depend on the size of the tooth and the application in which the cycloid drive is used.
[0056] Figure 6B illustrates a cycloid drive with rolling contact diameter passing through a midpoint of cycloid segments of partial cycloid teeth, in accordance with an example implementation. In Figure 6B, the planet gear 600 and the ring gear 604 are shown with numerous, partial cycloid teeth, as opposed to the full cycloid teeth shown in Figure 6A. As illustrated in Figure 6B, rolling contact diameters 608 and 610 of the planet gear 600 and the ring gear 604, respectively, pass through the midpoint of the cycloid segments of the teeth. Thus, the meshing teeth tend to slide less and have a minimum pressure angle. Efficiency of the cycloid drive is therefore increased.
V. Compensating for Eccentricity
[0057] As mentioned above, a planet gear of cycloid drives is affixed or coupled to an eccentric shaft. An output shaft of the cycloid drive is coupled to the planet gear of the cycloid drive, and therefore the output shaft has eccentric motion and displaces perpendicular to the gear rotational axis. In order to transmit a concentric angular rotation, the displacement has to be removed.
[0058] Figure 7 illustrates a mechanism that compensates for eccentric motion of an output shaft of a cycloid drive, in accordance with an example implementation. An input shaft 700
is coupled to an eccentrically mounted bearing 702. The bearing 702 drives a cycloidal disk (planet gear) 704. The cycloidal disk 704 has a number of holes such as hole 706. These holes provide surfaces for output shaft rollers, such as output shaft roller 708, to roll thereon. The output shaft rollers are coupled to an output shaft (not shown in Figure 7). Radius of the a hole, such as the hole 706, is larger than radius of a corresponding output shaft roller, such as the roller 708, by the amount of eccentricity.
[0059] With this configuration, as the input shaft 700 is rotated, due to the eccentricity of the bearing 702, the cycloid disk 704 rotates in an eccentric manner. As the cycloid disk 704 rotates, it applies force on the output shaft rollers, e.g., the output shaft roller 708, causing the output shaft rollers to rotate. Due to the holes (e.g., the hole 706) being larger than the output shaft rollers (e.g., the output shaft roller 708) by the amount of eccentricity, the eccentricity is removed and the output shaft is imparted with a circular, non-eccentric motion.
[0060] The mechanism shown in Figure 7, however, may be characterized by having a large number of precision parts. Disclosed next are alternative mechanisms with a fewer number of parts compared to the mechanism shown in Figure 7.
[0061] Figure 8 illustrates a coupling 800 used to connect two shafts that are not aligned coaxially, in accordance with an example embodiment. The coupling 800 includes three disks 802, 804, and 806. One of the outer disks such as the disk 802 may be coupled to an input shaft while the other outer disk 806 may be coupled to an output shaft.
[0062] The middle disk 804 is coupled to both outer disks by tongue (i.e., key) and groove (i.e., keyway) configurations as shown. The terms "tongue" and "key" are used interchangeably herein. Similarly, the terms "groove" and "keyway" are used interchangeably herein.
[0063] Specifically, the outer disk 802 has a groove 808 and the middle disk 804 has a tongue 810 on a side facing the outer disk 802 and thus corresponds to and engages with the groove 808. Similarly, the middle disk 804 has a groove 812 on a side that faces the outer disk 806, and the outer disk 806 has a tongue 814 that corresponds to and engages with the groove 812. The tongue 810 is perpendicular to the groove 812. Accordingly, the middle disk 804 is configured to slide radially with respect to the outer disks 802 and 806 as the mechanism rotates.
[0064] The unaligned input and output shafts are coupled to the outer disks 802 and 806 and the middle disk 804 transfers rotation of the input shaft to the output shaft. Because the
middle disk 804 is configured to slide radially with respect to the outer disks 802 and 806, the effect of the misalignment between the input and output shafts is eliminated.
[0065] The coupling 800 could be used to eliminate the eccentricity of cycloid drives. Compared to the mechanism described with respect to Figure 7, the coupling 800 is has less number of parts.
[0066] As an example, referring back to Figure 4D, one of the outer disks 802 and 806 of the coupling 800 may be coupled to the planet gear 404. The output shaft may then be coupled to the other outer disk. Thus, as the planet gear 404 rotates in an eccentric manner, the ability of the middle disk 804 to slide radially with respect to the outer disks 802 and 806 compensates for the effect of the eccentricity at the output shaft.
[0067] Figures 9A-9B illustrates a coupling configuration 900 to compensate for eccentricity at an output of a cycloid drive, in accordance with an example implementation. In this configuration, in contrast to the relatively large tongue and groove arrangement illustrated in Figure 8, an array of smaller tongues and grooves are utilized. By using multiple parallel smaller tongues and grooves, the load capacity of the coupling increases for a given volume, thus enabling the mechanism to be more compact for a give load capacity.
[0068] Figures 9A-9B illustrate a cycloid drive with its planet gear and ring gear having partial cycloid teeth as described above with respect to Figures 4A-4D. The cycloid drive further has multiple parallel tongues and grooves for removing the eccentricity from the output of the cycloid drive.
[0069] Figure 9A shows an exploded view of the cycloid drive with one viewing angle and Figure 9B shows an exploded view from another viewing angle so that both sides of the components may be illustrated in the Figures. The input shaft may be coupled to component 901 at a center of the component 901(i.e., the input shaft and the component 901 are concentric). A bearing 902 is eccentrically mounted to the input component 901. The eccentrically mounted bearing 902 is coupled to a planet gear 904. The planet gear 904 has partial cycloid teeth 906 that mesh with partial cycloid teeth 908 of a ring hear 910.
[0070] Further, as shown in Figure 9B, the planet gear 904 operates as one of the output disks 802 and 806. The planet gear 904 has a first side that faces toward the input shaft and a second side opposite to the first side. The second side includes multiple tongues and grooves 911 as opposed to a single tongue (e.g., the tongue 814) or a single groove (e.g., the groove 808).
[0071] The configuration 900 includes an intermediate disk 912 that is equivalent to the middle disk 804 in Figure 8. Instead of the single tongue 810 and the single groove 812 of the disk 804, the disk 912 has multiple tongues and grooves 914 and 916 on both sides of the disk. A first side of the disk 912 faces toward the planet gear 904 and has the tongues and grooves 914, whereas a second side opposite to the first side has the tongues and grooves 916. The tongues and grooves 914 are perpendicular to tongues and grooves 916.
[0072] Disk 918 is an output disk similar to either of the outer disks 802 and 806. The disk 918 has multiple tongues or groove 920 configured to engage with the tongues or grooves 916 of the disk 912. In operation, as the planet gear 904 moves in an eccentric manner, the disk 912 slides radially with respect to both the planet gear 904 and the output disk 918, and thus the eccentricity of the output is eliminated. The configuration 900 shown in Figures 9A- 9B includes fewer parts compared to the mechanism shown in Figure 7, and could thus be more cost effective.
[0073] Figures 10A-10B illustrates a configuration 1000 to compensate for eccentricity at an output of a cycloid drive, in accordance with an example implementation. The configuration 1000 uses links to compensate for the eccentricity.
[0074] An input shaft may be coupled to an eccentrically mounted bearing 1002. The bearing 1002 is eccentric with respect to the input shaft as described in previous configurations. The configuration 1000 includes a planet gear 1004 having partial cycloid teeth 1006. A ring gear 1008 also has the partial cycloid teeth 1010. The planet gear 1004 has a first side facing toward the input shaft and a second side opposite the first side.
[0075] The configuration 1000 includes four links 1012A, 1012B, 1012C, and 1012D, each link having two pegs. More or fewer links could be used, and each link could have more or fewer pegs. The links 1012A, 1012B, 1012C, and 1012D are connected or coupled to each other and are disposed in a plane parallel to a respective plane of the planet gear 1004. The pegs of the links 1012A, 1012B, 1012C, and 1012D protrude in a direction perpendicular to the plane.
[0076] The configuration 1000 also has an intermediate member 1014 having four holes as shown. The configuration 1000 also has an output member 1016 that has two holes, such as hole 1018.
[0077] A subset the pegs of the links 1012A, 1012B, 1012C, and 1012D face toward and are coupled to the intermediate member 1014 and output member 1016, whereas another subset of pegs face toward and are coupled to the planet gear 1004.
[0078] The dashed lines in Figure 10B illustrate how half of the pegs of the links 1012A, 1012B, 1012C, and 1012D are coupled to holes in other members. For instance, a peg 1020 of the link 1012D extends beyond the intermediate member 1014 and is coupled to the hole 1018 of the output member 1016. A peg 1022 of the link 1012D is coupled to a hole 1024 of the intermediate member 1014. A peg 1026 of the link 1012B is coupled to a hole 1028 of the intermediate member 1014. A peg 1030 of the link 1012B is coupled to a hole 1032 of the planet gear 1004. Only half the connections of the pegs with respective holes are shown to reduce visual clutter in the drawings.
[0079] Each peg is free to rotate within a corresponding hole the peg is received at or coupled thereto. As described in previous configurations, the planet gear 1004 moves about in an eccentric manner. The lengths of the links 1012A, 1012B, 1012C, and 1012D should be substantially larger than the amount of eccentricity of the planet gear 1004 so as to compensate for the eccentricity. The planet gear 1004 causes, via the pegs coupled to the planet gear 1004, the links 1012A-D and the intermediate member 1014 to move in a manner that eliminates or reduces the eccentric motion. Thus, the output member 1016 also moves about without the eccentricity. A shaft coupled to the output member would therefore rotate without eccentric motion. Similar to the configuration shown in Figures 9A-9B, the configuration shown in Figures 10A-10B includes fewer parts compared to the mechanism shown in Figure 7, and requires fewer precision machining operations, and could thus be more cost effective.
[0080] Figure 11 illustrates another configuration 1100 to compensate for eccentricity of a cycloid drive, in accordance with an example implementation. While the configurations shown previously include a single planet gear, the configuration 1100 includes a compound planet gear 1101 having two planet gears 1102 and 1104. The two planet gears 1102 and 1104 are affixed to each other, and thus rotate as one unit at the same speed.
[0081] The configuration 1100 also include two corresponding ring gears 1106 and 1108, such that the planet gear 1102 meshes with the ring gear 1106 and the planet gear 1104 meshes with ring gear 1108. One of the ring gears is grounded, i.e., fixed, while the other ring gear is free to rotate, i.e., floating.
[0082] Pitch diameters of the two planet gears 1102 and 1104 are different by a small or threshold amount. For example, pitch diameter of the planet gear 1102 could be 55 millimeter (mm) and pitch diameter of the planet gear 1104 could be 50 mm. Similarly, pitch diameter of the two ring gears 1106 and 1108 are different by a small or threshold amount, but the difference in pitch diameters of the ring gears is equal to the difference in the pitch diameters of the planet gears. For example, pitch diameter of the ring gear 1106 could be 60 mm and pitch diameter of the planet gear 1108 could be 55 mm.
[0083] Figure 11 also shows an input shaft 1110 coupled to an eccentric component 1112, which is coupled to the planet gears 1102 and 1104. A roller bearing 1114 is configured to encompass the eccentric component 1112. In operation, as the input shaft 1110 rotates, the planet gears 1102 and 1104 both move in an eccentric manner within their respective ring gears 1106 and 1108, respectively.
[0084] If the ring gear 1106 is considered as the "ground" gear (i.e., the gear that does not move), then the output may be harvested from the ring gear 1108, which is free to rotate or is floating. The arrangement of the planet gear 1104 and ring gear 1108 cancels the eccentricity of the rotation of planet gear 1102 within the ring gear 1106. Thus, the output has no eccentricity. In this configuration, a large gear ratio reduction may be obtained as the gear ratio is the product of the two gear ratios between each ring and planet pair. Further, similar to the configurations shown in Figures 9A-9B and Figures 10A-10B, the configuration shown in Figure 11 includes fewer parts compared to the mechanism shown in Figure 7, and could thus be more cost effective.
V. Conclusion
[0085] It should be understood that arrangements described herein are for purposes of example only. As such, those skilled in the art will appreciate that other arrangements and other elements (e.g., machines, interfaces, orders, and groupings of operations, etc.) can be used instead, and some elements may be omitted altogether according to the desired results.
[0086] While various aspects and implementations have been disclosed herein, other aspects and implementations will be apparent to those skilled in the art. The various aspects and implementations disclosed herein are for purposes of illustration and are not intended to be limiting, with the true scope being indicated by the following claims, along with the full scope of equivalents to which such claims are entitled. It is also to be understood that the
terminology used herein is for the purpose of describing particular implementations only, and is not intended to be limiting.